Amplifier interface and amplification methods for ultrasound devices

ABSTRACT

Amplifier architecture that allows low-cost class-D audio amplifiers to be compatible with ultrasonic signals, as well as loads presented by thin-film ultrasonic transducers. The amplifier architecture replaces the traditional capacitor used as an output filter in the class-D amplifier with the natural capacitance of the ultrasonic transducer load, and employs relative impedance magnitudes to create an under-damped low-pass filter that boosts voltage in the ultrasonic frequency band of interest. The amplifier architecture includes a secondary feedback loop to ensure that correct output voltage levels are provided.

CROSS REFERENCE TO RELATED APPLICATIONS

This patent application is a continuation of U.S. patent applicationSer. No. 15/859,905 filed Jan. 2, 2018 entitled AMPLIFIER INTERFACE ANDAMPLIFICATION METHODS FOR ULTRASOUND DEVICES, which claims benefit ofthe priority of U.S. Provisional Patent Application No. 62/441,468 filedJan. 2, 2017 entitled AMPLIFIER INTERFACE AND METHODS FOR ULTRASOUND.

BACKGROUND

Amplifying ultrasonic signals has traditionally been both challengingand costly. The frequency range required for such amplification isbeyond most audio amplifier capabilities, and the highly capacitive loadpresented by an ultrasonic transducer is significantly different fromthe weakly inductive and mostly resistive load presented by aloudspeaker. Further, for many ultrasonic transducers, a much higherdrive voltage (e.g., about 200-300 Vpp) is required compared with thedrive voltage required for loudspeakers. For at least these reasons,ultrasonic amplifiers, whether designed to be linear or switching, aregenerally custom made to suit a specific application and/or device.

Class-D amplifiers were once relegated to subwoofer use, but are nowcapable of reproducing signals in the audio frequency band (i.e.,20-20,000 Hz) with good fidelity and at low cost, due in no small partto advancements made in the field of semiconductor technology. Recentclass-D amplifier designs compatible with 192 kHz sample rate audiosignals are now theoretically capable of driving up to one-half of thissample rate, or 96 kHz, which is well into a useful ultrasound frequencyrange. Such class-D amplifier designs are desirable because they arecurrently being manufactured in high quantities, and are generallyavailable at low cost in a convenient “module” amplifier package, whichtypically includes signal processing, pulse width modulation, switchdriving, power semiconductors, as well as amplifier protection andfeedback correction. However, while such class-D amplifier designstheoretically allow high-frequency ultrasound reproduction, theygenerally do not permit practical use with ultrasonic transducers orparametric loudspeaker systems.

SUMMARY

In accordance with the present application, amplifier architecture isdisclosed that allows low-cost class-D audio amplifiers to be compatiblewith ultrasonic signals, as well as loads presented by thin-filmultrasonic transducers. The disclosed amplifier architecture replacesthe traditional capacitor used as an output filter in the class-Damplifier with the natural capacitance of the ultrasonic transducerload, and employs relative impedance magnitudes to create anunder-damped low-pass filter that boosts voltage in the ultrasonicfrequency band of interest. The disclosed amplifier architectureincludes a secondary feedback loop to ensure that correct output voltagelevels are provided.

In certain embodiments, an amplifier interface for driving an ultrasonictransducer includes a switching amplifier configured to receive anultrasonic signal from an ultrasonic source, and one or more inductancescoupled between the switching amplifier and the ultrasonic transducer.The ultrasonic transducer has a transducer capacitance. The amplifierinterface further includes processing circuitry associated with theultrasonic source, and a feedback path disposed between the ultrasonictransducer and the processing circuitry. The feedback path is configuredto provide, to the processing circuitry, a signal representative of anoutput level of the ultrasonic transducer. The processing circuitry isconfigured to correct the output level of the ultrasonic transducer inresponse to variations in one or more values of the one or moreinductances and the transducer capacitance.

In certain embodiments, an amplifier interface for driving an ultrasonictransducer includes a switching amplifier configured to receive anultrasonic signal, and a first inductance coupled between the switchingamplifier and the ultrasonic transducer. The ultrasonic transducer has atransducer capacitance. The first inductance and the transducercapacitance are configured to form a filter having a frequency response.The amplifier interface further includes a second inductance in parallelwith the ultrasonic transducer. One or more values of the secondinductance and the transducer capacitance are selected to reduce acurrent draw in the frequency response of the filter within anultrasonic frequency band of interest.

Other features, functions, and aspects of the invention will be evidentfrom the Detailed Description that follows.

BRIEF DESCRIPTION OF THE DRAWINGS

The foregoing and other objects, features, and advantages will beapparent from the following description of particular embodiments of theinvention, as illustrated in the accompanying drawings in which likereference characters refer to the same parts throughout the differentviews.

FIG. 1a is a schematic diagram of a conventional amplifier interface fordriving a loudspeaker;

FIG. 1b is a diagram of an exemplary frequency response provided by theamplifier interface of FIG. 1 a;

FIG. 2a is a schematic diagram of an exemplary amplifier interface fordriving an ultrasonic transducer;

FIG. 2b is a diagram of an exemplary frequency response provided by theamplifier interface of FIG. 2a ; and

FIG. 3 is a diagram of a practical frequency response and phase responseprovided by the amplifier interface of FIG. 2 a.

DETAILED DESCRIPTION

The disclosures of U.S. patent application Ser. No. 15/859,905 filedJan. 2, 2018 entitled AMPLIFIER INTERFACE AND AMPLIFICATION METHODS FORULTRASOUND DEVICES and U.S. Provisional Patent Application No.62/441,468 filed Jan. 2, 2017 entitled AMPLIFIER INTERFACE AND METHODSFOR ULTRASOUND are hereby incorporated herein by reference in theirentirety.

Amplifier architecture is disclosed that allows low-cost class-D audioamplifiers to be compatible with ultrasonic signals, as well as loadspresented by thin-film ultrasonic transducers. The disclosed amplifierarchitecture replaces the traditional capacitor used as an output filterin the class-D amplifier with the natural capacitance of the ultrasonictransducer load, and employs relative impedance magnitudes to create anunder-damped low-pass filter that boosts voltage in the ultrasonicfrequency band of interest. The disclosed amplifier architectureincludes a secondary feedback loop to ensure that correct output voltagelevels are provided.

FIG. 1a depicts an illustrative embodiment of a conventional amplifierinterface 100 for driving a loudspeaker 110. As shown in FIG. 1a , theamplifier interface 100 includes a class-D (switch mode type) amplifier104, and a pair of low-pass (L-C) filters 105.1, 105.2. The low-passfilter 105.1 includes an inductor 106.1 and a capacitor 108.1. Likewise,the low-pass filter 105.2 includes an inductor 106.2 and a capacitor108.2. In the illustrative embodiment of FIG. 1a , the class-D amplifier104 can be configured to include a full-bridge (or H-bridge) outputstage, which provides a pair of outputs (Output 1, Output 2) for drivingthe loudspeaker 110. It is noted, however, that the class-D amplifier104 may alternatively be configured to include a half-bridge outputstage or any other suitable output stage configuration.

In an exemplary mode of operation, an audio source 102 produces an audiosignal in the audio frequency band (i.e., 20-20,000 Hz), and providesthe audio signal to an input of the class-D amplifier 104, whichincludes suitable components for synthesizing and amplifying pulse widthmodulated (PWM) signals based on the audio input signal, as known in theart. The PWM signals include the audio signal to be reproduced at theloudspeaker 110, as well as high frequency switching artifacts outsidethe audible frequency band. The class-D amplifier 104 provides a PWMsignal at each of its Outputs 1, 2, which, in turn, provide therespective PWM signals to the low-pass filters 105.1, 105.2. Thelow-pass filter 105.1 is configured to filter the PWM signal at theOutput 1 of the class-D amplifier 104 to remove the high frequencyswitching artifacts from the respective PWM signal. Likewise, thelow-pass filter 105.2 is configured to filter the PWM signal at theOutput 2 of the class-D amplifier 104 to remove the high frequencyswitching artifacts from the respective PWM signal. Having removed thehigh frequency switching artifacts from the PWM signals, the low-passfilters 105.1, 105.2 provide the audio signal in the audio frequencyband to the loudspeaker 110 for subsequent reproduction.

FIG. 1b depicts an exemplary frequency response 112 of the low-passfilters 105.1, 105.2 included in the amplifier interface 100 of FIG. 1a. As shown in FIG. 1b , the cutoff frequency, Fc, of the low-passfilters 105.1, 105.2 can be expressed, as follows:

$\begin{matrix}{{{Fc} = \frac{1}{2\pi\sqrt{LC}}},} & (1)\end{matrix}$in which “L” corresponds to the inductance value of the inductors 106.1,106.2, and “C” corresponds to the capacitance value of the capacitors108.1, 108.2. It is noted that, for a full-band audio device, the cutofffrequency Fc is typically about 20 kHz.

For enhanced accuracy and lower distortion, the class-D amplifier 104can employ real-time feedback (generally depicted by arrows 111.1,111.2; see FIG. 1a ) derived from its output stage. The class-Damplifier 104 can process (e.g., filter) the real-time feedback, comparethe processed feedback to the audio input signal, and employ a resultingerror function to suppress distortion and enhance reproduction accuracy.Because the output filter is flat in the audio frequency band ofinterest, it is generally not necessary to obtain such feedback from theload presented by the loudspeaker 110, as the output from the class-Damplifier is representative and accurate, at least within the audiofrequency band of interest.

FIG. 2a depicts an illustrative embodiment of an amplifier interface 200for driving an ultrasonic transducer 214, in accordance with the presentapplication. As shown in FIG. 2a , the amplifier interface 200 includesa class-D (switch mode type) amplifier 204, a transformer 206, aninductor 208, a DC bias circuit 211, and a peak detector 210. The DCbias circuit 211 includes an isolation capacitor 212, an isolationresistor 216, and a DC bias generator 218. The transformer 206 isconfigured to provide isolation and a ground reference, and to allow theimpedance seen by the class-D amplifier 204 to be adjusted to a suitablerange, as well as allow the output voltage to be adjusted to a suitablelevel. In the illustrative embodiment of FIG. 2a , the class-D amplifier204 can be configured to include a full-bridge (or H-bridge) outputstage, which provides a pair of outputs (Output 1, Output 2) coupled toan input winding of the transformer 206. It is noted, however, that theclass-D amplifier 204 may alternatively be configured to include ahalf-bridge output stage or any other suitable output stageconfiguration. Further, for enhanced accuracy and lower distortion, theclass-D amplifier 204 can employ real-time feedback (generally depictedby one or more primary feedback paths 219.1, 219.2; see FIG. 2a )derived from its output stage. A compensation filter can also be used toflatten the net ultrasound response of the ultrasonic transducer 214.

The amplifier interface 200 for driving the ultrasonic transducer 214(see FIG. 2a ) can be contrasted with the conventional amplifierinterface 100 for driving the loudspeaker 110 (see FIG. 1a ), at leastas follows. First, the capacitance provided by the capacitors 108.1,108.2 included in the low-pass filters 105.1, 105.2 is replaced by thenatural capacitance of the ultrasonic transducer 214. This eliminatesthe need for the capacitors 108.1, 108.2, and, by reducing the totalcapacitance, reduces the amount of current that the class-D amplifier204 is required to supply to drive the ultrasonic transducer 214 to adesired voltage level. The capacitance of the ultrasonic transducer 214can be trimmed by adding a capacitor of a relatively small capacitancevalue, preferably in parallel with the ultrasonic transducer 214, suchthat the cutoff frequency Fc (see FIG. 2b ) is located in a desiredultrasound frequency range. In addition, the inductance value of theinductor 208 is selected such that a resulting frequency response 222(see FIG. 2b ) has a cutoff frequency, Fc, located approximately in thecenter of the ultrasonic frequency band of interest. The inductance ofthe inductor 208 can be trimmed, as desired and/or required, usingtunable inductor devices or one or more additional inductors in seriesor parallel. Because the resistance of the load presented by theultrasonic transducer 214 is low, the inductance of the inductor 208 andthe natural capacitance of the ultrasonic transducer 214 create anunder-damped (or “peaking”) low-pass filter, as illustrated by thefrequency response 222 of FIG. 2b . As shown in FIG. 2b , a strongresonance peak is created at approximately the cutoff frequency Fc,thereby naturally amplifying the output voltage in the desiredultrasonic frequency band. In FIG. 2b , a frequency response 220 (shownin phantom) similar to the frequency response 112 of FIG. 1b is shownfor comparison with the under-damped or peaking frequency response 222.

It is noted that the strong resonance peak at the cutoff frequency Fc(see FIG. 2b ) allows the frequency response 222 to have characteristicsof a band-pass filter. It is further noted that, near the cutofffrequency Fc (see FIG. 2b ), the series-resonance combination of theinductor 208 and the natural capacitance of the ultrasonic transducer214 presents a load to the class-D amplifier 204 that appears to bemostly resistive, thereby making the ultrasonic transducer 214compatible with standard class-D amplifier modules designed for use withresistive loads.

Because the under-damped or peaking low-pass filter created by theinductance of the inductor 208 and the natural capacitance of theultrasonic transducer 214 does not have a flat frequency response, andthe inductance value of the inductor 208 and the capacitance/resistancevalue(s) of the ultrasonic transducer 214 may vary and/or drift, theamplifier interface 200 is configured to include a secondary feedbackpath 209 from a node between the inductor 208 and the capacitor 212 toan ultrasonic source/digital signal processor (DSP) coupled to an inputof the class-D amplifier 204. It is noted that the change in phase nearthe cutoff frequency Fc (see FIG. 2b ) can be rapid, and therefore adirect feedback comparison with the output of the amplifier interface200 can be difficult to implement. For this reason, a slower feedbackloop implemented by the secondary feedback path 209 with a signalrepresentative of the output level is employed.

As described herein, the inductance, L, of the inductor 208 and thenatural capacitance, C, of the ultrasonic transducer 214 create anunder-damped or peaking low-pass filter, as illustrated by the frequencyresponse 222 of FIG. 2b . In one embodiment, the ultrasonic transducer214 is configured as a thin-film ultrasonic transducer, in which theinternal series resistance is relatively small compared to the impedanceof L and C in the ultrasound frequency range of interest. Such athin-film ultrasonic transducer generally requires a high voltage (and aDC bias) for proper operation. For this reason, the broadband, flatfrequency response of the class-D amplifier 204 is effectively convertedinto a band-pass frequency response with voltage boost, which is usefulfor amplifying band-limited ultrasonic signals centered at the cutofffrequency, Fc, as expressed as in equation (1) above. The magnitude ofthe voltage boost near the cutoff frequency, Fc, is dependent upon therelative values of L, C, as well as the load resistance. It is notedthat there can be a tradeoff between the useful bandwidth and themagnitude of the voltage boost. In an exemplary configuration of theamplifier interface 200, a 24 Vdc power supply can be used to drive theultrasonic transducer load to 200-500 Vpp near the cutoff frequency, Fc,allowing maximum drive limits of the ultrasonic transducer load to bereached over a reasonable bandwidth. It is further noted that a carrierfrequency of a modulated ultrasonic signal produced by the ultrasonictransducer 214 can be selected to be near the cutoff frequency, Fc. Forcertain types of ultrasonic signal modulation, such as single side-band(SSB), the cutoff frequency, Fc, can be approximately at the center ofthe ultrasonic frequency band of interest.

FIG. 3 depicts an illustrative phase response 302 and frequency response304 of the under-damped or peaking low-pass filter created by theinductance, L, of the inductor 208, and the natural capacitance, C, ofthe ultrasonic transducer 214. Exemplary values of the inductance, L, ofthe inductor 208, the natural capacitance, C, of the ultrasonictransducer 214, as well as the internal series resistance of theultrasonic transducer 214, are 80 uH, 100 nF, and 2Ω, respectively. Asshown in FIG. 3, the frequency response 304 provides a voltage boost ofabout 23 dB at a cutoff frequency (Fc) of about 56 kHz, thereby boostingthe voltage level at the ultrasonic transducer load by a factor of overten (10) and, for nearby frequencies, providing a voltage boost of abouta factor of four (4) or more over a bandwidth of about 14 kHz. Becausethe frequency response 304 rolls off at higher frequencies, highfrequency switching harmonics are effectively eliminated (i.e., filteredout) from the output of the class-D amplifier 204. It is noted thatproper selection of the inductance, L, of the inductor 208 inconjunction with the natural capacitance, C, of the ultrasonictransducer 214 ensures that the load seen by the class-D amplifier 204is mostly resistive, at least in the ultrasonic frequency band ofinterest. The class-D amplifier 204, which is typically designed for usewith resistive loads, can therefore be used to drive the load of theultrasonic transducer 214 at high voltage both efficiently and at lowcost.

As described herein, the transformer 206 can be included in theamplifier interface 200 of FIG. 2a to provide isolation and a groundreference, and to allow the impedance seen by the class-D amplifier 204to be adjusted to a suitable range. More specifically, in the case wherethe class-D amplifier 204 is configured to include a full-bridge (orH-bridge) output stage, the transformer 206 can effectively convert adifferential driving capability of the full-bridge output stage to asingle-ended, ground-referenced output signal, without sacrificing theoutput voltage amplitude. Moreover, the transformer 206 can beconfigured as a step-up or step-down transformer to tailor the maximumvoltage swing at the output, as well as alter the impedance seen by theclass-D amplifier 204, thereby ensuring that the class-D amplifier 204is operating within appropriate current limits and at the rated loadimpedance.

As further described herein, the class-D amplifier 204 can employreal-time feedback (generally depicted by the primary feedback path(s)219.1, 219.2; see FIG. 2a ) from its output stage for enhanced accuracyand lower distortion. Such feedback, which is typically provided inoff-the-shelf class-D amplifier modules, is useful in conventionalarchitectures such as the amplifier interface 100 (see FIG. 1a ),because the cutoff frequency, Fc, of the output filter tends to be welloutside the audio frequency band of interest, and the signal seen by theload presented by the loudspeaker 110 is about the same as that seen atthe output of the class-D amplifier 104, at least within the audiofrequency band of interest. In the architecture of the amplifierinterface 200 (see FIG. 2a ), however, an under-damped resonance iscreated between the class-D amplifier 204 and the load presented by theultrasonic transducer 214, so the amplitude of the signal seen by theultrasonic transducer load is different from that seen by theloudspeaker load and is highly frequency dependent. Further, the phaseresponse 302 changes rapidly in the ultrasonic frequency band ofinterest, and therefore a direct feedback of the signal at the output ofthe amplifier interface 200 is difficult to implement. For this reason,rather than using the entire output signal for feedback purposes, theamplifier interface 200 employs a signal representative of the outputlevel in the secondary feedback path 209. In the amplifier interface 200of FIG. 2a , such a signal is provided by the peak detector 210 to anultrasonic source/digital signal processor (DSP) 202 to ensure that thesignal seen by the ultrasonic transducer load has accurate amplitude,especially with variations in the values of inductance, L, and thecapacitance, C. Because the secondary feedback path 209 can include anonlinear element (e.g., the peak detector 210) rather than a linearfilter, such feedback provided by the secondary feedback path 209 can beviewed as being nonlinear. It should be noted, however, that afull-signal, linear filtered, or any other suitable secondary feedbackpath may be employed. In an alternative embodiment, the peak detector210 can be replaced with a rectifier or any other suitablesignal-conditioning configuration. For higher-speed DSP interfaces, thenonlinear element 210 can be omitted, and the requisite signalconditioning can be performed within the DSP (see reference numeral 202)for the secondary feedback path 209.

The DC bias circuit 211 can apply a suitable DC bias voltage (e.g., 250Vdc) to the ultrasonic transducer 214 for increased sensitivity andmaximum output. In the amplifier interface 200 of FIG. 2a , the DC biasgenerator 218 feeds the DC bias voltage through the resistor 216, whichprotects the DC bias generator 218 from a high voltage AC drive signalseen by the ultrasonic transducer load. Further, the capacitor 212 isconfigured to block the DC bias voltage from the class-D amplifier 204,as well as the transformer 206. The capacitor 212 is provided with acapacitance value suitably high enough to avoid substantiallyinfluencing the high voltage AC drive signal being fed to the ultrasonictransducer 214. In an alternative embodiment, the capacitor 212 can belocated between the transformer 206 and the inductor 208, and thefeedback provided by the secondary feedback path 209 can be obtaineddirectly from the ultrasonic transducer load.

As still further described herein, a compensation filter can be used toflatten the net ultrasound response of the ultrasonic transducer 214.More specifically, the compensation filter can be used to compensate forthe non-flat frequency response 222 (see FIG. 2b ) in the vicinity ofthe cutoff frequency, Fc. Such a compensation filter can be implementedby the ultrasonic source/DSP 202, which can be configured to measure thefrequency response 222 using the output level provided via secondaryfeedback path 209. It is noted that the compensation filter can beeither fixed to provide a correction for expected values of inductance(L) and/or capacitance (C), or adjustable to account for possible driftin the values of inductance (L) and/or capacitance (C).

In one mode of operation, the ultrasonic source/DSP 202 produces anultrasonic signal in the ultrasonic frequency band (i.e., 50-70 kHz),and provides the ultrasonic signal to an input of the class-D amplifier204, which can include a full-bridge output stage. The transformer 206converts the differential driving capability of the full-bridge outputstage to a single-ended, ground-referenced output signal, and providesthe output signal to the under-damped or peaking low-pass filter createdby the inductance of the inductor 208 and the natural capacitance of theultrasonic transducer 214, which can be a thin-film ultrasonictransducer. The peak detector 210 provides a signal representative ofthe output level via the secondary feedback path 209 to the ultrasonicsource/DSP 202, which uses the output level to compensate for thenon-flat frequency response of the under-damped or peaking low-passfilter near the cutoff frequency, Fc. The DC bias circuit 211 applies asuitable DC bias voltage to the thin-film ultrasonic transducer forincreased sensitivity and maximum output.

Having described the above illustrative embodiments of the amplifierinterface 200 (see FIG. 2a ) and associated amplification methods forultrasonic devices, other variations and/or modifications can be madeand/or practiced. For example, the amplifier interface and amplificationmethods described herein can be employed in a parametric loudspeakersystem configured (i) to receive an audio input signal, (ii) to processthe audio signal using a DSP, (iii) to modulate the audio signal to theultrasonic frequency band using a carrier frequency near the cutofffrequency, Fc, and (iv) to deliver the modulated ultrasonic signal tothe amplifier interface 200 for reproduction by the ultrasonictransducer 214. An ultrasonic output produced by the ultrasonictransducer 214 is then demodulated by the nonlinear characteristics ofthe propagation medium (e.g., the air), converting the ultrasonic outputinto audible sound that can be heard by a human subject.

It was described herein that the amplifier interface 200 incorporatingthe class-D amplifier 204 can be used to drive the ultrasonic transducer214. In an alternative embodiment, the amplifier interface 200 can beused to drive any suitable reactive load, such as an antenna(capacitive) or a coil or motor (inductive—the positions of capacitance,C, and inductance, L, are reversed). In another alternative embodiment,the amplifier interface 200 can be configured to incorporate a class-Aamplifier, a class-B amplifier, a class-T amplifier, or any othersuitable amplifier normally used to amplify audio signals. In a furtheralternative embodiment, one or more transient-voltage-suppression (TVS)diodes can be used at the output of the amplifier interface 200 toprotect the class-D amplifier 204 from damage due to current spikes thatmay cause voltage ripples to reflect back through the amplifierinterface circuit, potentially reaching the class-D amplifier 204.

As further described herein, the carrier frequency of the modulatedultrasonic signal produced by the ultrasonic transducer 214 can beselected to be near the cutoff frequency, Fc. In an alternativeembodiment, such a carrier frequency can be adjusted to enhance thevoltage boost of the frequency response of the amplifier interface 200,thereby accounting for inherent variations in the inductance of theinductor 208 and/or the natural capacitance of the ultrasonic transducer214. In such an alternative embodiment, the carrier frequency can beadjusted at the ultrasonic source/DSP 202 either dynamically duringoperation or during programmed calibration sequences (such as uponstartup), based on the signal representative of the output levelprovided via the secondary feedback path 209. In a further alternativeembodiment, the frequency response 222 of the amplifier interface 200can be tuned by (i) inserting one or more additional resistors in thesignal chain to reduce the peak of the frequency response 222, and/or(ii) inserting one or more inductors and/or capacitors in the signalchain to move the position of the peak of the frequency response 222, aswell as the frequency region affected by the voltage boost provided bythe frequency response 222, etc.

It was further described herein that the amplifier interface 200 caninclude the series inductor 208. In an alternative embodiment, theseries inductor 208 can be replaced with a secondary inductance in thetransformer 206, or an inductor disposed in parallel with the ultrasonictransducer load, resulting in a flat voltage response and reducedcurrent consumption at frequencies close to where the inductance of theinductor 208 and the natural capacitance of the ultrasonic transducer214 are resonant. In such an alternative embodiment, another low-passfilter (e.g., another L-C filter) can be added before or after thetransformer 206, either separately or combined with the inductance ofthe transformer 206.

While various embodiments of the invention have been particularly shownand described, it will be understood by those skilled in the art thatvarious changes in form and details may be made therein withoutdeparting from the scope of the invention as defined by the appendedclaims.

What is claimed is:
 1. An amplifier interface for driving an ultrasonictransducer, comprising: a switching amplifier configured to receive anultrasonic signal from an ultrasonic source; one or more inductancescoupled between the switching amplifier and the ultrasonic transducer,the ultrasonic transducer having a transducer capacitance; processingcircuitry associated with the ultrasonic source; and a feedback pathdisposed between the ultrasonic transducer and the processing circuitry,wherein the feedback path is configured to provide, to the processingcircuitry, a signal representative of an output level of the ultrasonictransducer, and wherein the processing circuitry is configured tocorrect the output level of the ultrasonic transducer in response tovariations in one or more values of the one or more inductances and thetransducer capacitance.
 2. The amplifier interface of claim 1 whereinthe one or more inductances and the transducer capacitance areconfigured to form a filter for reducing high frequency artifactsproduced by the switching amplifier.
 3. The amplifier interface of claim1 wherein the feedback path includes one of a peak detector and arectifier.
 4. The amplifier interface of claim 1 further comprising: atransformer disposed between the switching amplifier and the ultrasonictransducer.
 5. The amplifier interface of claim 1 wherein the ultrasonictransducer is a thin-film ultrasonic transducer.
 6. The amplifierinterface of claim 1 wherein the one or more values of the one or moreinductances and the transducer capacitance are selected to provide aresonance near an ultrasonic frequency band of interest.
 7. Theamplifier interface of claim 6 wherein the resonance is configured toprovide a voltage boost in the ultrasonic frequency band of interest. 8.The amplifier interface of claim 6 wherein the resonance is configuredto minimize a current draw in the ultrasonic frequency band of interest.9. The amplifier interface of claim 6 wherein one or more values, L, ofthe one or more inductances and a value, C, of the transducercapacitance are selected such that ${{Fc} = \frac{1}{2\pi\sqrt{LC}}},$wherein “Fc” approximates an ultrasonic frequency band of interest. 10.An amplifier interface for driving an ultrasonic transducer, comprising:a switching amplifier configured to receive an ultrasonic signal; afirst inductance coupled between the switching amplifier and theultrasonic transducer, the ultrasonic transducer having a transducercapacitance, wherein the first inductance and the transducer capacitanceare configured to form a filter having a frequency response; and asecond inductance in parallel with the ultrasonic transducer, whereinone or more values of the second inductance and the transducercapacitance are selected to reduce a current draw in the frequencyresponse of the filter within an ultrasonic frequency band of interest.11. The amplifier interface of claim 10 wherein the ultrasonictransducer is a thin-film ultrasonic transducer.
 12. The amplifierinterface of claim 11 further comprising: a DC bias circuit configuredto provide a DC bias voltage to the thin-film ultrasonic transducer. 13.The amplifier interface of claim 12 wherein the DC bias circuit includesan isolation capacitor configured to block the DC bias voltage, andwherein the isolation capacitor is disposed in series with theultrasonic transducer.
 14. The amplifier interface of claim 12 whereinthe DC bias circuit includes a DC bias generator and an isolationresistor, and wherein the isolation resistor is disposed between the DCbias generator and the ultrasonic transducer.
 15. The amplifierinterface of claim 10 wherein the one or more values of the secondinductance and the transducer capacitance are selected to provide aresonance near a frequency band of interest.
 16. The amplifier interfaceof claim 15 wherein the ultrasonic transducer is configured to receive asignal modulated by an ultrasonic carrier frequency, and wherein theultrasonic carrier frequency is within the frequency band of interest.17. The amplifier interface of claim 10 further comprising: atransformer disposed between the switching amplifier and the ultrasonictransducer.
 18. The amplifier interface of claim 17 wherein thetransformer has one or more transformer windings, and wherein the one ormore transformer windings are configured to provide the secondinductance.
 19. The amplifier interface of claim 17 wherein thetransformer is configured to adjust an impedance seen by the switchingamplifier to within a predetermined impedance range.
 20. The amplifierinterface of claim 19 wherein the transformer is configured as a step-uptransformer to increase voltage levels delivered to the ultrasonictransducer.